Please use this identifier to cite or link to this item: http://nopr.niscair.res.in/handle/123456789/14911
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dc.contributor.authorPatil, B J-
dc.contributor.authorPatil, A J-
dc.contributor.authorChavan, S T-
dc.contributor.authorPethe, S N-
dc.contributor.authorKrishnan, R-
dc.contributor.authorBhoraskar, V N-
dc.contributor.authorDhole, S D-
dc.date.accessioned2012-11-05T10:14:36Z-
dc.date.available2012-11-05T10:14:36Z-
dc.date.issued2012-11-
dc.identifier.issn0975-1041 (Online); 0019-5596 (Print)-
dc.identifier.urihttp://hdl.handle.net/123456789/14911-
dc.description814-817en_US
dc.description.abstractFLUKA simulation has been carried out using 15 MeV LINAC to design thermal neutron source for radiography. In this case, a neutron collimator has been designed along with e- target, -n target, moderator and shielding. The -n target has been optimized based on their photonuclear reaction threshold. The moderating properties have been studied for a few light elements to optimize best suitable moderator for radiography system. To get best values of collimator parameters such as collimation ratio, gamma content, neuron fluence rate, cadmium ratio, beam uniformity etc., a FLUKA simulation was carried out. The collimator has been optimized with cadmium lining square cone to capture the scattered thermal neutrons and the collimation ratio to L/D=20. The neutron fluence rate and neutron to gamma ratio of the optimized facility at the object plane is 1.1 105 n cm-2 s-1 and 1.0 105 n cm-2 mR-1.en_US
dc.language.isoen_USen_US
dc.publisherNISCAIR-CSIR, Indiaen_US
dc.rights CC Attribution-Noncommercial-No Derivative Works 2.5 Indiaen_US
dc.sourceIJPAP Vol.50(11) [November 2012]en_US
dc.subjectNeutron radiographyen_US
dc.subjectFLUKA simulationen_US
dc.subjectThermal neutron sourceen_US
dc.subjectLinear acceleratoren_US
dc.subject-n targeten_US
dc.titleFLUKA simulation of 15 MeV linear accelerator based thermal neutron source for radiographyen_US
dc.typeArticleen_US
Appears in Collections:IJPAP Vol.50(11) [November 2012]

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